4 research outputs found
Conflict between the Electronic Factors and Structure-Directing Rules in the Intergrowth Structure of Ca<sub>4</sub>Ag<sub>2+<i>x</i></sub>Ge<sub>4–<i>x</i></sub> with <i>x</i> = 1/2
Combined experimental
and theoretical efforts to conceptually understand
the structure directing forces in intergrowth structures have led
to the discovery of the new ternary phase Ca<sub>4</sub>Ag<sub>2+<i>x</i></sub>Ge<sub>4<i>–x</i></sub> (<i>x</i> = 0.5), obtained from high-temperature reaction of the
elements. It crystallizes in a new structure type according to single-crystal
diffraction methods: monoclinic space group <i>C</i>2/<i>m–i</i><sup>10</sup> with <i>a</i> = 10.7516(2)
Å, <i>b</i> = 4.5475(1) Å, <i>c</i> =
18.7773(4) Å, β = 93.69(2)°, <i>V</i> =
916.17(3) Å<sup>3</sup>, <i>Z</i> = 4. The compound
corresponds to the <i>n</i> = 2 member of the homologous
series Ca<sub>2+<i>n</i></sub>Ag<sub>2+<i>x</i></sub>Ge<sub>2+<i>n–x</i></sub>, that are built
up by linear intergrowths of slabs cut from the CaGe (CrB-type) and
the CaAg<sub>1+<i>x</i></sub>Ge<sub>1<i>–x</i></sub> (KHg<sub>2</sub> or TiNiSi-type) structures, and may be partitioned
in Ag-rich and Ag-free domains. Instead of the predicted Zr<sub>2</sub>CoSi<sub>2</sub>-type (<i>C</i>2/<i>m–i</i><sup>5</sup>), a simultaneous doubling of the size of the two building
blocks is observed with the dimerization of the (Ge<sub>2</sub>) pairs
into Ag-substituted tetramers (Ag<sub><i>x</i></sub>Ge<sub>4<i>–x</i></sub>) due to valence electron shortage.
However, the Ag/Ge mixing at one atomic site with roughly one-to-one
atomic ratio is therefore unexplained. The electronic band structure
calculations and analysis of the chemical bonding provided evidence
that the Ag/Ge mixing is rather the result of a direct conflict between
the Zintl-Klemm concept and empirically established “structure-directing
rules”. The implications of these findings for the poorly understood
ordered staging structural interfaces, typically observed in secondary
Li-ion batteries during charge/discharge process, are briefly discussed
Drastic Change of Magnetic Interactions and Hysteresis through Site-Preferential Ru/Ir Substitution in Sc<sub>2</sub>FeRu<sub>5–<i>x</i></sub>Ir<sub><i>x</i></sub>B<sub>2</sub>
The
quinary members of the complex boride series Sc<sub>2</sub>FeRu<sub>5–<i>x</i></sub>Ir<sub><i>x</i></sub>B<sub>2</sub> were synthesized by arc melting the elements
and characterized by powder and single-crystal X-ray diffraction as
well as metallographic and energy-dispersive X-ray analyses. The use
of a 4d/5d mixture allows distinguishing these elements with X-ray
diffraction methods, thus enabling the study of site preference and
its influence on the magnetic properties.The magnetic measurements
reveal several changes of magnetic ordering
within the series: from antiferromagnetism (Sc<sub>2</sub>FeRu<sub>5</sub>B<sub>2</sub>) to ferromagnetism (Sc<sub>2</sub>FeRuIr<sub>4</sub>B<sub>2</sub>) and finally to metamagnetism (Sc<sub>2</sub>FeIr<sub>5</sub>B<sub>2</sub>). Within the quinary series, the magnetic
moments continuously increase with increasing amounts of Ir in one
(8<i>j</i>) of two possible Wyckoff sites. The members with <i>x</i> = 2 and 3 represent the first hard magnetic borides of
transition metals
A Stacking Faults-Containing Silicogermanate with 24-Ring Channels and Unbranched <i>Zweier</i> Silica Double Chains
A novel open-framework silicogermanate SU-JU-14 (Stockholm
University-Jilin
University-Number 14), |NH<sub>3</sub>CH<sub>2</sub>CH<sub>2</sub>NH<sub>3</sub>|<sub>3</sub>[Ge<sub>6.40</sub>Si<sub>0.60</sub>O<sub>15</sub>(OH)]<sub>2</sub>[Ge<sub>0.73</sub>Si<sub>3.27</sub>O<sub>8</sub>], was synthesized
by using ethylenediamine as the structure-directing agent under solvothermal
conditions. Single-crystal structure analysis reveals that the crystal
structure of SU-JU-14 consists of extended 24-ring channels built
from [(Ge,Si)<sub>7</sub>O<sub>12</sub>O<sub>6/2</sub>(OH)]<sup>3–</sup> [(Ge,Si)<sub>7</sub>] clusters and unbranched <i>zweier</i> silica double chains [Ge<sub>0.73</sub>Si<sub>3.27</sub>O<sub>4</sub>O<sub>8/2</sub>]. Charge neutrality is achieved by diprotonated ethylenediamine
guest molecules. The structure consists of stacking faults of layered
arrays in two different configurations along the <i>a</i>-axis. SU-JU-14 was characterized by X-ray diffraction, X-ray energy
dispersive spectroscopy, scanning electron microscopy, nuclear magnetic
resonance, inductively coupled plasma, and thermogravimetric analyses.
Crystallographic data: monoclinic, space group <i>C</i>2/<i>c</i>, and unit cell parameters: <i>a</i> = 35.625
(7) Å, <i>b</i> = 28.580 (6) Å, <i>c</i> = 10.403 (2) Å, and β = 98.30 (3)°
A Stacking Faults-Containing Silicogermanate with 24-Ring Channels and Unbranched <i>Zweier</i> Silica Double Chains
A novel open-framework silicogermanate SU-JU-14 (Stockholm
University-Jilin
University-Number 14), |NH<sub>3</sub>CH<sub>2</sub>CH<sub>2</sub>NH<sub>3</sub>|<sub>3</sub>[Ge<sub>6.40</sub>Si<sub>0.60</sub>O<sub>15</sub>(OH)]<sub>2</sub>[Ge<sub>0.73</sub>Si<sub>3.27</sub>O<sub>8</sub>], was synthesized
by using ethylenediamine as the structure-directing agent under solvothermal
conditions. Single-crystal structure analysis reveals that the crystal
structure of SU-JU-14 consists of extended 24-ring channels built
from [(Ge,Si)<sub>7</sub>O<sub>12</sub>O<sub>6/2</sub>(OH)]<sup>3–</sup> [(Ge,Si)<sub>7</sub>] clusters and unbranched <i>zweier</i> silica double chains [Ge<sub>0.73</sub>Si<sub>3.27</sub>O<sub>4</sub>O<sub>8/2</sub>]. Charge neutrality is achieved by diprotonated ethylenediamine
guest molecules. The structure consists of stacking faults of layered
arrays in two different configurations along the <i>a</i>-axis. SU-JU-14 was characterized by X-ray diffraction, X-ray energy
dispersive spectroscopy, scanning electron microscopy, nuclear magnetic
resonance, inductively coupled plasma, and thermogravimetric analyses.
Crystallographic data: monoclinic, space group <i>C</i>2/<i>c</i>, and unit cell parameters: <i>a</i> = 35.625
(7) Å, <i>b</i> = 28.580 (6) Å, <i>c</i> = 10.403 (2) Å, and β = 98.30 (3)°